Frequency of Virbration in Covalent Bonds

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SUMMARY

The frequency of vibration in covalent bonds cannot be determined solely from bond energy and bond length. To find vibrational frequencies, one must analyze the potential-energy curve E(r) through second-order derivatives at the equilibrium point, where first-order derivatives equal zero. Higher-order derivatives are necessary for anharmonic corrections. A full quantum-mechanical calculation is required to accurately derive E(r), and approximations like the Lennard-Jones potential can only provide limited insights based on experimental data.

PREREQUISITES
  • Understanding of harmonic oscillator models in quantum mechanics
  • Familiarity with potential-energy curves and their derivatives
  • Knowledge of quantum-mechanical calculations for covalent bonds
  • Experience with fitting experimental data to theoretical models, such as the Lennard-Jones potential
NEXT STEPS
  • Study harmonic oscillator eigenfrequencies and their derivation from potential-energy curves
  • Learn about quantum-mechanical calculations for covalent bond energies
  • Research the Lennard-Jones potential and its applications in molecular modeling
  • Explore the LCAO (Linear Combination of Atomic Orbitals) model and its use in fitting overlap integrals
USEFUL FOR

Chemists, physicists, and materials scientists interested in molecular vibrations, covalent bond analysis, and quantum mechanics will benefit from this discussion.

sritter27
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I came across an interesting problem involving covalent bonds that I'm having trouble solving. If you're given a bond energy and a bond length, how would you find the frequency of vibration of the covalent bond? I tried to approach this through dimensional analysis and I'm not seeing how I would get a frequency out of this.
 
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You can't.

If you know the energy as a function of bond length E(r), then you can determine the harmonic-oscillator eigenfrequencies from the second-order derivatives of E with respect to r, taken at the equilibrium point, where the first-order derivatives (forces) are zero. Getting anharmonic corrections requires even higher-order derivatives.

Or, to put it another way, the vibrational frequencies depend on (and are in fact a kind of description of) the potential-energy curve E(r) of the bond distance. You need to know the whole curve to know the frequencies. If you only know the energy and bond length, all you have is a single point on the curve. The simplest way to get the information about it is to determine the derivatives as above, in what's essentially a Taylor expansion around the equilibrium point.

You can't get E(r) with anything less than a full quantum-mechanical calculation.
 
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The best you could do is fit an idealized potential.

For example, if you think about the Lennard-Jones potential. There are two parameter that are fit from experiment. If you have the position and energy of the minima then you have enough to make the potential fit.

If you knew that it was s-valent you could fit the overlap integral for a LCAO model. In is textbook David Pettifor suggests that you can use a power series to describe the integral's dependence on r. Walter Harrison also had some useful function forms in his book, I think. Of course you don't have enough information to fit anything with p or d orbitals.

Of course both of these approximations are severe and wouldn't stand in a research setting.
 
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